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CN112909570A - Three-dimensional broadband wave-absorbing metamaterial integrating multiple absorption mechanisms - Google Patents

Three-dimensional broadband wave-absorbing metamaterial integrating multiple absorption mechanisms Download PDF

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Publication number
CN112909570A
CN112909570A CN202110164786.0A CN202110164786A CN112909570A CN 112909570 A CN112909570 A CN 112909570A CN 202110164786 A CN202110164786 A CN 202110164786A CN 112909570 A CN112909570 A CN 112909570A
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metamaterial
dimensional
plate
absorbing
wave
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CN112909570B (en
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刘亚青
韩冠宇
樊益泽
苏晓岗
赵贵哲
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North University of China
Shanxi Zhongbei New Material Technology Co Ltd
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North University of China
Shanxi Zhongbei New Material Technology Co Ltd
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q15/00Devices for reflection, refraction, diffraction or polarisation of waves radiated from an antenna, e.g. quasi-optical devices
    • H01Q15/0006Devices acting selectively as reflecting surface, as diffracting or as refracting device, e.g. frequency filtering or angular spatial filtering devices
    • H01Q15/0086Devices acting selectively as reflecting surface, as diffracting or as refracting device, e.g. frequency filtering or angular spatial filtering devices said selective devices having materials with a synthesized negative refractive index, e.g. metamaterials or left-handed materials
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q17/00Devices for absorbing waves radiated from an antenna; Combinations of such devices with active antenna elements or systems

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Abstract

The invention belongs to the technical field of electromagnetic functional materials, and particularly relates to a three-dimensional broadband wave-absorbing metamaterial integrating multiple absorption mechanisms; the three-dimensional broadband wave-absorbing metamaterial is an array of three-dimensional metamaterial units, each row at least comprises two three-dimensional metamaterial units, and each column at least comprises two three-dimensional metamaterial units; the three-dimensional metamaterial unit comprises an upper dielectric slab, a lower dielectric slab and a metal bottom plate which are sequentially arranged from top to bottom, wherein a high magnetic loss material plate is embedded in the midpoint of the inner part of the lower dielectric slab, and the lower surfaces of the upper dielectric slab and the lower dielectric slab are tightly attached to the upper surface of the metal bottom plate; the conductor core is embedded in the center of the upper dielectric plate, and the lower surfaces of the conductor core and the lower dielectric plate are tightly attached to the upper surface of the lower dielectric plate. By introducing the conductor core into the all-dielectric metamaterial and using materials with different loss capacities at different parts, the prepared wave-absorbing metamaterial has the loss mechanism of the traditional metamaterial and the step-type all-dielectric metamaterial, the effective absorption bandwidth is expanded, and the use of high-loss materials can be reduced.

Description

Three-dimensional broadband wave-absorbing metamaterial integrating multiple absorption mechanisms
Technical Field
The invention belongs to the technical field of electromagnetic functional materials, and particularly relates to a three-dimensional broadband wave-absorbing metamaterial integrating multiple absorption mechanisms, which can be used for broadband microwave absorption.
Background
The traditional metamaterial wave absorber mainly absorbs waves through electromagnetic resonance of a metamaterial metal structure, when electromagnetic waves are incident on the surface of the metamaterial structure, an electric field enables a surface metal array to play a role of an electric resonator, and meanwhile, a magnetic field enables the surface metal array and a bottom metal substrate to play a role of a magnetic resonator. By adjusting the unit shape and the structural parameters of the metal array, the impedance of the metamaterial wave absorber at the resonance frequency and the free space can be matched, so as to minimize the reflection of the incident electromagnetic wave, such as the metamaterial wave absorber formed by the metal wires and the semiconductor wafers in patent CN 201110061836.9. However, the impedance of the conventional metamaterial wave absorber can only be matched with the free space in a very narrow range near the resonant frequency, so that the wave absorbing bandwidth is very narrow and is difficult to meet the practical application.
The step-type all-dielectric metamaterial mainly utilizes multiple lambda/4 resonance to achieve the purpose of phase cancellation, utilizes corner diffraction and coupling effect among units to concentrate electromagnetic waves, achieves good impedance matching, and further utilizes a loss medium to absorb, such as the step-type all-dielectric metamaterial provided by patent CN 201610989091.5. Although broadband absorption is easy to realize, the metamaterial has high requirement on the loss capacity of the dielectric material, and is not beneficial to industrial popularization and application.
Disclosure of Invention
The invention overcomes the defects of the prior art, provides the metamaterial for absorbing the electromagnetic waves based on multiple absorption mechanisms, leads the conductor core into the ladder-shaped all-dielectric metamaterial, uses materials with different loss capacities at different parts, ensures that the prepared wave-absorbing metamaterial has the loss mechanisms of the traditional metamaterial and the ladder-shaped all-dielectric metamaterial, only locally uses high-loss materials while expanding the effective absorption bandwidth, can effectively reduce the cost, and is beneficial to industrial popularization and application.
In order to solve the technical problems, the technical scheme adopted by the invention is as follows:
a three-dimensional broadband wave-absorbing metamaterial integrating multiple absorption mechanisms is an array of three-dimensional metamaterial units, each row at least comprises two three-dimensional metamaterial units, and each column at least comprises two three-dimensional metamaterial units; the three-dimensional metamaterial unit comprises an upper dielectric plate, a lower dielectric plate and a metal bottom plate which are sequentially arranged from top to bottom, wherein a high magnetic loss material plate is embedded in the center of the interior of the lower dielectric plate, and the lower surfaces of the upper dielectric plate and the lower dielectric plate are tightly attached to the upper surface of the metal bottom plate; a conductor core is embedded in the center of the upper dielectric plate, and the lower surfaces of the upper dielectric plate and the lower dielectric plate are tightly attached to the upper surface of the lower dielectric plate; all metal bottom plates are spliced together, and all lower dielectric slabs are respectively positioned on the same horizontal plane.
Further, the upper and lower dielectric plates are in a regular quadrangular prism shape, wherein the side length a of the lower dielectric plate 315-25 mm in height h11-5.5 mm, the side length a of the upper dielectric plate 425-25 mm in height h2Is 1-5.5 mm, and a1>a2The dielectric constants of the upper dielectric plate and the lower dielectric plate are both 4-8.
Further, the conductor core 5 is a regular cross prism, which is a regular prism having a cross-shaped cross section, and has a length b11-5.5 mm, width b21-5.5 mm, height h41-5.5 mm, and b1>b2,a2>b1, h2≥h4(ii) a The conductor core 5 is made of a metal material or a carbon material.
Preferably, the metal material is copper, aluminum or silver; the carbon material is graphite or carbon black.
Further, the high magnetic loss material plate 2 is in a regular quadrangular prism shape with a side length b35-25 mm in thickness h3Is 1-5.5 mm, and a1>b3,h1>h3The dielectric constant of the high-magnetic loss material plate 2 is 12-13, and the magnetic conductivity is 1-3.
Furthermore, the upper and lower dielectric plates and the high magnetic loss material plate 2 are all made of resin-based wave-absorbing composite materials.
Furthermore, the resin-based wave-absorbing composite material is composed of a resin matrix, a curing agent and a filled wave-absorbing agent.
Furthermore, the resin matrix is epoxy resin, the curing agent is amine or anhydride curing agent, and the filled wave absorbing agent is carbon material, magnetic material or composite multi-element particles of the carbon material and the magnetic material.
Preferably, the carbon material is graphene or carbon nanotubes; the magnetic material is ferroferric oxide, carbonyl iron or alpha-Fe.
Compared with the prior art, the invention has the following beneficial effects:
1) the conductor core is introduced into the periodic loss medium, so that the metamaterial-based resonant cavity has various absorption mechanisms such as traditional metamaterial electric resonance, magnetic resonance, ladder-type full-medium metamaterial lambda/4 resonance, edge diffraction and the like, and the filled conductor core is also beneficial to forming capacitors among units, strengthening the coupling effect among the units and improving the impedance matching effect. Therefore, the effective absorption bandwidth is as high as 13.57 GHz.
(2) According to the invention, because the part which generates magnetic resonance and concentrates a magnetic field between the conductor core and the bottom layer metal substrate is filled with the high magnetic loss material, the magnetic field energy can be accurately absorbed, the using amount of the high magnetic loss material can be reduced, the cost is effectively reduced, and the industrial popularization and application are facilitated.
(3) Due to the excellent symmetrical structure, the invention has certain polarization insensitivity and good large-angle incidence stability under TM polarization, and can keep the broadband absorption with the effective absorption bandwidth of 13.57 GHz within the incidence angle range of 0-60 degrees in the TM polarization mode.
The invention has the structural characteristics of the ladder-type all-dielectric metamaterial and introduces the conductor core, can concentrate incident electromagnetic waves by various absorption mechanisms and pertinently lose the incident electromagnetic waves, so that the broadband effective absorption in the range of 4.43-18 GHz is realized while only locally using a high-magnetic-loss material, and the ladder-type all-dielectric metamaterial has certain polarization insensitivity and incident angle stability; in addition, the method also has the advantages of low cost, contribution to industrial popularization and application and the like.
Drawings
FIG. 1 is a schematic view of an overall structure of a three-dimensional broadband wave-absorbing metamaterial integrating multiple absorption mechanisms.
FIG. 2 is a schematic diagram of a unit structure of a three-dimensional broadband wave-absorbing metamaterial integrating multiple absorption mechanisms.
Fig. 3 is a perspective view of fig. 2.
Fig. 4 is a top view of fig. 2.
Fig. 5 is a side sectional view of fig. 2.
Fig. 6 is a graph showing the simulation result of the reflection loss in the TE polarization mode at an incident angle of 0 ° in the present invention.
Fig. 7 is a graph showing simulation results of reflection loss in the TM polarization mode at an incident angle of 0 ° in the present invention.
FIG. 8 is a graph showing the simulation results of reflection loss in the TM polarization mode at an incident angle of 0-60 deg. according to the present invention.
The figures are labeled as follows:
1-metal bottom plate, 2-high magnetic loss material plate, 3-lower dielectric plate, 4-upper dielectric plate and 5-conductor core.
Detailed Description
The present invention is further illustrated by the following specific examples.
Examples
As shown in FIG. 1, the present embodiment is formed by M × N three-dimensional metamaterial units with multiple absorption mechanisms periodically arranged, wherein M is greater than or equal to 2, N is greater than or equal to 2, and M and N are positive integers.
As shown in fig. 2 and 3, each three-dimensional metamaterial unit includes a metal base plate 1, a high-magnetic-loss material plate 2, a lower dielectric plate 3, an upper dielectric plate 4, and a conductor core 5.
The high magnetic loss material plate 2 is embedded in the center of the lower dielectric plate 3, and the lower surfaces of the high magnetic loss material plate and the lower dielectric plate are tightly attached to the upper surface of the metal bottom plate 1 with the thickness of 0.035 mm; the conductor core 5 is embedded in the center of the upper dielectric plate 4, and the lower surfaces of the conductor core and the upper dielectric plate are tightly attached to the center of the upper surface of the lower dielectric plate 3.
As shown in FIGS. 4 and 5, the lower dielectric sheet 3 has a regular quadrangular prism shape with a side length a1Is 15 mm and has a height h12.5 mm and a relative dielectric constant of 4-8.
As shown in fig. 5, the high magnetic loss material plate 2 has a regular quadrangular prism shape, and the bottom surface thereof is flush with the bottom surface of the lower dielectric plate 3 and is fitted in the center of the lower dielectric plate 3. Side length b thereof3Is 13.2 mm and has a height h30.9mm, dielectric constant of 12-13 and magnetic permeability of 1-3.
The upper dielectric plate 4 is in the shape of a regular quadrangular prism with a side length a29.5mm, height h23.5mm and a relative dielectric constant of 4-8.
As shown in fig. 4, the upper surface of the conductor core 5 is flush with the upper surface of the upper dielectric plate 4 and is embedded in the center of the upper dielectric plate 4. It is in the shape of a regular cross prism and has a length of b1Is 5mm and has a width b2Is 1.5 mm and has a height h4Is 3.5 mm.
All of the metals mentioned above in this example are aluminum, but are not limited thereto.
The specific wave absorbing principle of the three-dimensional metamaterial integrating multiple absorption mechanisms in the embodiment is as follows:
when electromagnetic waves are incident to the metamaterial in the embodiment, the stepped structure formed by the lower dielectric plate 3 and the upper dielectric plate 4 can generate lambda/4 resonance with different frequencies at different thicknesses, so that the electromagnetic waves are subjected to coherence cancellation; the polygonal structure can generate edge diffraction effect, change the propagation direction of incident electromagnetic wave, make it enter the loss medium more easily, and propagate longer path. The side surfaces of the upper dielectric plate 4 and the conductor core 5 between different units can accumulate positive and negative charges under the action of an electromagnetic field, and can be equivalent to a series of capacitors, so that the electric field energy is concentrated between the units and is lost by a loss medium.
The conductor core 5 embedded in the upper dielectric plate 4 can generate electric resonance under the action of an electric field, and the electric field is concentrated around the metal and absorbed by a loss medium; the lower surface of the metal bottom plate and the metal bottom plate 1 can generate magnetic resonance under the action of a magnetic field, the magnetic field is concentrated between the lower surface of the metal bottom plate and the metal bottom plate, and the metal bottom plate is lost through the high-magnetic-loss material plate 2 embedded in the lower dielectric plate 3.
The technical effects of the invention are further explained by combining simulation experiments as follows:
1. simulation software:
business simulation software CST microwave studio 2018
2. Simulation content and results:
simulation 1, simulation software is used to perform simulation calculation on the reflection loss of the three-dimensional metamaterial, which integrates multiple absorption mechanisms, in the frequency range of 2-18 GHz and when TE polarized incident waves are vertically incident, that is, the incident angle is equal to 0 °, and the result is shown in fig. 6.
As can be seen from FIG. 6, when the TE polarization mode is adopted and the incident angle is equal to 0 °, the minimum reflection loss of the three-dimensional metamaterial integrating a plurality of absorption mechanisms in one body in the present example is-17.67 dB, and the effective absorption frequency band with the reflection loss less than-10 dB is from 4.43 GHz to 18 GHz.
Simulation 2, simulation software is used to perform simulation calculation on reflection loss of the three-dimensional metamaterial integrating multiple absorption mechanisms in the embodiment when the three-dimensional metamaterial is vertically incident in the frequency range of 2-18 GHz, namely when the incident angle is equal to 0 °, and the result is shown in fig. 7.
As can be seen from FIG. 7, when the TM polarization mode is adopted and the incident angle is equal to 0 °, the minimum reflection loss of the three-dimensional metamaterial integrating multiple absorption mechanisms in one body in the present example is-17.95 dB, and the absorption frequency band with the reflection loss smaller than-10 dB is from 4.43 GHz to 18 GHz. This is consistent with the results in the TE polarization mode, indicating that the present invention has polarization insensitive properties.
Simulation 3, simulation software is used for carrying out simulation calculation on the reflection loss of the three-dimensional metamaterial integrating multiple absorption mechanisms in the embodiment within the frequency range of 2-18 GHz and TM polarized incident waves, namely, within the incident angle range of 0-60 degrees, and the result is shown in fig. 8.
As can be seen from fig. 8, in the TM polarization mode, the effective absorption band range with a reflection loss less than-10 dB remains substantially unchanged, and as the incident angle increases, the reflection loss value gradually decreases, and the minimum reflection loss achieved at an incident angle of 60 ° is-25.23 dB. This shows that the present invention has an incident angle stability in the incident angle range of 0-60 deg. in the TM polarization mode.
The above description and examples are only preferred embodiments of the present invention and should not be construed as limiting the present invention, it will be obvious to those skilled in the art that various modifications and changes in form and detail may be made based on the principle and construction of the present invention after understanding the content and design principle of the present invention, but such modifications and changes based on the inventive concept are still within the scope of the appended claims.

Claims (9)

1. The three-dimensional broadband wave-absorbing metamaterial is characterized in that the three-dimensional broadband wave-absorbing metamaterial is an array of three-dimensional metamaterial units, each row at least comprises two three-dimensional metamaterial units, and each column at least comprises two three-dimensional metamaterial units; the three-dimensional metamaterial unit comprises an upper dielectric slab (4), a lower dielectric slab (3) and a metal bottom plate (1) which are sequentially arranged from top to bottom, wherein a high-magnetic-loss material plate (2) is embedded in the center of the interior of the lower dielectric slab (3), and the lower surfaces of the upper dielectric slab and the lower dielectric slab are tightly attached to the upper surface of the metal bottom plate (1); a conductor core (5) is embedded in the center of the upper dielectric plate (4), and the lower surfaces of the upper dielectric plate and the lower dielectric plate are tightly attached to the upper surface of the lower dielectric plate (3); all the metal bottom plates (1) are spliced together, and all the lower-layer dielectric plates (3) are respectively positioned on the same horizontal plane.
2. The three-dimensional broadband wave-absorbing metamaterial integrating multiple absorption mechanisms as claimed in claim 1, wherein the upper and lower dielectric plates are all in a regular quadrangular prism shape, wherein the side length a of the lower dielectric plate (3) is15-25 mm in height h11-5.5 mm, the side length a of the upper dielectric plate (4)25-25 mm in height h2Is 1-5.5 mm, and a1>a2The dielectric constants of the upper dielectric plate and the lower dielectric plate are both 4-8.
3. The three-dimensional broadband wave-absorbing metamaterial according to claim 2, wherein the conductor core (5) is in the shape of a regular cross prism, the regular cross prism is a regular prism with a cross-shaped cross section, and the length b of the regular cross prism is larger than that of the conductor core11-5.5 mm, width b21-5.5 mm, height h41-5.5 mm, and b1>b2,a2>b1,h2≥h4(ii) a The conductor core (5) is made of a metal material or a carbon material.
4. The three-dimensional broadband wave-absorbing metamaterial according to claim 3, wherein the metal material is copper, aluminum or silver; the carbon material is graphite or carbon black.
5. The three-dimensional broadband wave-absorbing metamaterial integrating multiple absorption mechanisms as claimed in claim 2, wherein the high-magnetic-loss material plate (2) is in a regular quadrangular prism shape with a side length b35-25 mm in thickness h3Is 1-5.5 mm, and a1>b3,h1>h3The dielectric constant of the high-magnetic-loss material plate (2) is 12-13, and the magnetic conductivity is 1-3.
6. The three-dimensional broadband wave-absorbing metamaterial integrating multiple absorption mechanisms according to any one of claims 1, 2 or 5, wherein the upper and lower dielectric plates and the high-magnetic-loss material plate (2) are made of resin-based wave-absorbing composite materials.
7. The three-dimensional broadband wave-absorbing metamaterial integrating multiple absorption mechanisms according to claim 6, wherein the resin-based wave-absorbing composite material is composed of a resin matrix, a curing agent and a filled wave-absorbing agent.
8. The three-dimensional broadband wave-absorbing metamaterial integrated with multiple absorption mechanisms according to claim 7, wherein the resin matrix is epoxy resin, the curing agent is amine or anhydride curing agent, and the filled wave-absorbing agent is carbon material, magnetic material or multi-element particles compounded by the carbon material and the magnetic material.
9. The three-dimensional broadband wave-absorbing metamaterial integrated with multiple absorption mechanisms according to claim 8, wherein the carbon material is graphene or carbon nanotubes; the magnetic material is ferroferric oxide, carbonyl iron or alpha-Fe.
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CN114336083A (en) * 2021-12-27 2022-04-12 杭州电子科技大学 Dual-polarized broadband absorbing frequency selective structure based on two- and three-dimensional inter-embedded structure
CN115173080A (en) * 2022-07-28 2022-10-11 合肥工业大学 Tunable terahertz metamaterial wave absorber
CN118693526A (en) * 2024-03-29 2024-09-24 杭州市钱塘区信息高等研究院 A phase-programmable three-dimensional metamaterial unit
CN119181980A (en) * 2024-11-01 2024-12-24 南京林业大学 Low-profile dual-polarized electromagnetic metamaterial absorber with ultra-wideband wave absorbing characteristic

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CN115173080A (en) * 2022-07-28 2022-10-11 合肥工业大学 Tunable terahertz metamaterial wave absorber
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CN119181980A (en) * 2024-11-01 2024-12-24 南京林业大学 Low-profile dual-polarized electromagnetic metamaterial absorber with ultra-wideband wave absorbing characteristic

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